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The copolymers with crystallised structures were transparent, had a low glass transition temperature of the polyether phase and a modulus that was independent of temperature between Tg and Tm.
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Two types of Ti-containing alloys were chosen as an object for coating: Ti-6Al-4V (recommended for orthopedic application) and a novel highly biocompatible Ti-Zr-Nb alloy, with good mechanical compatibility due to a modulus that is more close to that of human bones (E ≈ 50 GPa instead of 110 GPa in Ti-6Al-4V).
Transient viscosities during start-up of shear flow at extremely low shear rates are governed by very long relaxation times and by a modulus that is nearly the same as the plateau modulus obtained from oscillatory shear experiments.
We report the ultimate tensile strength as a modulus, that is, tissue property per cross-sectional area.
However for any modulus that is a power pn of a prime, it can be shown that there exists a unique multiplication making the group Zpn a ring in a way that makes the nonzero elements of the ring a cyclic (and therefore abelian) group under the multiplication, and hence making the ring a field.
A high content of guluronic acid resulted in a storage modulus that was almost three times greater than for the formulation with lower guluronic acid content in the case of gels formed using strontium alginate dispersions.
The formulation containing Gantrez S97 had a storage modulus that was significantly lower than PC in the gel state (temperatures above 16 °C) and in the lower temperature sol state.
In each material, an induction period was evident prior to an increase in modulus that was dependent on macromer chemistry (EGDMA < BDMA < PFDMA) that was primarily responsible for the difference in cure times.
Dynamical mechanical analysis was used to measure softening temperatures, and both the polystyrene-grafted and poly methyl methacrylate -grafted nanocomethacrylate -graftednanocompositesulus thad was higher than the correspeaking homopolymer, consisthet with strong polossr–lignin interactions.
This method is the introduction of a new pattern of shear modulus that was strictly derived according to the constitutive model based on the bimodular elasticity theory presented by Ambartsumyan.
Importantly, in this work we assume that water is an isotropic elastic solid with a shear modulus that is 10−4 times the bulk modulus of the water.
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